Figure 8
From: Electromagnetic wave transparency of X mode in strongly magnetized plasma
FFT of \(B_{z}\) with x at different times showing that as laser interacts with plasma, \(k_x\) shifts to a larger value than the initial \(k_x\). This shift reduces as we increase the magnitude of applied magnetic field (shown in different subplots). This shift in \(k_x\) is also reflected in velocity of EM wave approaching c in the medium (Table 4) and the transmission coefficient approaching unity (Table 3).
